JPH01142413A - Encoder apparatus - Google Patents

Encoder apparatus

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Publication number
JPH01142413A
JPH01142413A JP62300023A JP30002387A JPH01142413A JP H01142413 A JPH01142413 A JP H01142413A JP 62300023 A JP62300023 A JP 62300023A JP 30002387 A JP30002387 A JP 30002387A JP H01142413 A JPH01142413 A JP H01142413A
Authority
JP
Japan
Prior art keywords
elements
magnet
magnetic field
pitch
encoder device
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP62300023A
Other languages
Japanese (ja)
Inventor
Shigeru Ogino
滋 荻野
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canon Inc
Original Assignee
Canon Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP62300023A priority Critical patent/JPH01142413A/en
Publication of JPH01142413A publication Critical patent/JPH01142413A/en
Pending legal-status Critical Current

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  • Transmission And Conversion Of Sensor Element Output (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

PURPOSE:To obtain a plurality of signals from one MR element group, by differentiating and combining the saturated magnetic fields of the MR elements in accordance with specified rule. CONSTITUTION:A substrate 1 is arranged so as to face a magnet 2, which is magnetized in a specified pattern. MR elements 6 and 6' are formed on the substrate 1. The widths and the lengths of the MR elements 6 and 6' are different to each other. As a result, saturated magnetic fields are different. The MR elements 6 and 6' are aligned at a specified pitch and connected in series. In this constitution, a plurality of the MR elements 6 and 6' correspond to one magnetization of the magnet 2. Therefore, a plurality of output signals can be obtained. Since the pitch of the MR elements 6 and 6' can be determined accurately by a lithography technology, the detecting accuracy can be improved.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はエンコーダ装置に関し、特に磁気抵抗効果素子
(以下MR素子と称す)を用いるエンコーダ装置に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an encoder device, and particularly to an encoder device using a magnetoresistive element (hereinafter referred to as an MR element).

[従来の技術] 従来、この種のエンコーダ装置としては、磁気式のもの
と光学式のものとかあり、さらに磁気式エンコーダ装置
としては、磁気誘導によるコイル発電式のものやMR素
子を用いるものかある。
[Prior Art] Conventionally, there have been two types of encoder devices of this type: a magnetic type and an optical type.Furthermore, the magnetic encoder devices include a coil generation type using magnetic induction and a type using an MR element. be.

MR素子を用いたエンコーダ装置はN i−F e。An encoder device using an MR element is Ni-Fe.

Ni−Co5を薄膜形成法によりパターン化し、これら
薄膜素子の抵抗変化によって印加磁界の変化を検出する
。MR素子を用いたエンコーダ装置にあっては、永久磁
石等を被検出体の磁界発生手段として用いればよい。従
って、LED等の電源を必要とし、かつ消耗しつる光源
が不可欠なフォトセンサ等よりも構成か簡単でかつ耐久
性にも優れたエンコーダ装置が得られる。
Ni-Co5 is patterned by a thin film formation method, and changes in the applied magnetic field are detected by changes in resistance of these thin film elements. In an encoder device using an MR element, a permanent magnet or the like may be used as a magnetic field generating means for the detected object. Therefore, it is possible to obtain an encoder device that is simpler in construction and more durable than a photosensor or the like that requires a power source such as an LED, and also requires a consumable light source.

[発明が解決しようとする問題点] 上述の如きMR素子を用いたエンコーダ装置にあっては
、出力の分解能は1つの磁極に対して1つ、もしくは2
つの磁極に対して1つである。
[Problems to be Solved by the Invention] In the encoder device using the MR element as described above, the output resolution is one or two for one magnetic pole.
one for each magnetic pole.

従って、高分解能な出力を得るには永久磁石の単位反出
りの着磁数を増やす、即ち着磁ピッチを小さくする必要
がある。
Therefore, in order to obtain a high-resolution output, it is necessary to increase the number of magnetized permanent magnets per unit protrusion, that is, to reduce the magnetized pitch.

しかしながら、着磁ピッチを小さくすることには限界が
あり、さらにこれを高精度に行うことは困難である。そ
のため、高分解俺でかつ高精度のエンコーダを得ること
は困難であった。
However, there is a limit to reducing the magnetization pitch, and furthermore, it is difficult to do so with high precision. Therefore, it has been difficult to obtain an encoder with high resolution and high precision.

また、複数の出力信号を得るためには出力信号の数と同
数のMR素子を必要とするために、複数のMR素子を同
一基板上に配置することになる。
Furthermore, in order to obtain a plurality of output signals, the same number of MR elements as the number of output signals are required, so a plurality of MR elements are arranged on the same substrate.

ところが、多数のMR素子群を配置すると、装置全体が
大型化する。その上、MR素子か増すことにより引出し
パターンは増加し、その結果、多数のMR素子より得ら
れる出力信号を取出すための引出しパターンに対して、
MR素子に対向するマグネット等の磁界の移動により誘
起される起電力に基づくノイズが増加する。
However, arranging a large number of MR element groups increases the size of the entire apparatus. Furthermore, the number of extraction patterns increases as the number of MR elements increases, and as a result, for extraction patterns for extracting output signals obtained from a large number of MR elements,
Noise based on the electromotive force induced by the movement of the magnetic field of a magnet or the like facing the MR element increases.

本発明は上述の如き問題に鑑み、MR素子を用いたエン
コーダ装置において、これに高分解能でかつ高精度のエ
ンコーダにして複数の出力信号が得られることを可能な
らしめることを目的とする。
SUMMARY OF THE INVENTION In view of the above problems, it is an object of the present invention to provide a high-resolution and high-precision encoder device using an MR element, thereby making it possible to obtain a plurality of output signals.

[問題点を解決するための手段] かかる目的下において本発明のエンコーダ装置にあって
は、被検出体と検出体の相対位置を検出するエンコーダ
装置であって、所定ピッチで着磁された被検出体と、飽
和磁界が前記被検出体の着磁磁界に対し十分小さく、前
記着磁ピッチに比し小さいピッチで並列する複数の磁気
抵抗効果素子を前記被検出体に対向させ、前記並列する
複数の磁気抵抗効果素子の飽和磁界を所定の規則に異に
した検出体とを備えるものである。
[Means for Solving the Problems] In view of this objective, the encoder device of the present invention is an encoder device that detects the relative position of a detected object and a detected object, and which detects the relative position of a detected object and a detected object. A detection object and a plurality of magnetoresistive elements whose saturation magnetic field is sufficiently smaller than the magnetization magnetic field of the detection object and arranged in parallel at a pitch smaller than the magnetization pitch are placed opposite to the detection object and arranged in parallel. The detection body includes a plurality of magnetoresistive elements whose saturation magnetic fields are varied according to a predetermined rule.

[作用] 上述の如き構成にありては、着8i磁界か磁気抵抗効果
素子の飽和磁界より十分大きいので、該MR素子による
検出出力は急峻となり、かつ1つの着磁に対してそれ以
上のMR素子が対応するのて、分解能を高くし、かつ複
数の出力信号を得ることがてきる。また、MR素子のピ
ッチはフォトリソグラフィー技術により極めて正常に決
定できるため、検出精度の点ても向上する。
[Function] In the above configuration, since the magnetized 8i magnetic field is sufficiently larger than the saturation magnetic field of the magnetoresistive element, the detection output by the MR element becomes steep, and more MR Since the elements are compatible, resolution can be increased and multiple output signals can be obtained. Furthermore, since the pitch of the MR elements can be determined very accurately by photolithography, detection accuracy is also improved.

[実施例] 以下1本発明の実施例について説明する。[Example] An embodiment of the present invention will be described below.

第1図(a ) 、(b ) 、(c ) 、(d )
は本発明の第1の実施例である回転型エンコーダについ
て説明するための図であり、第1図(a)はこの回転型
エンコーダの断面図、同図(b)は被検出体であるとこ
ろのマグネットの着磁の様子を示す図、同図(c)は同
図(b)のマグネットの着磁信号を示す図、同図(d)
は検出体であるところのMR素子のパターンを示す図で
ある。
Figure 1 (a), (b), (c), (d)
1A and 1B are diagrams for explaining a rotary encoder that is a first embodiment of the present invention. FIG. 1A is a cross-sectional view of this rotary encoder, and FIG. (c) is a diagram showing the magnetization signal of the magnet in (b), (d) is a diagram showing how the magnet is magnetized.
1 is a diagram showing a pattern of an MR element which is a detection object.

第1図(a)においてマグネット2から出た磁束はMR
素子が成膜された基板lを通り、さらにステータヨーク
3を介して再び基板lを通ってマグネット2に戻る。マ
グネット2の着磁カーブとしては正弦波状9台形波状等
が考えられるか、以下は正弦波状であるものとして説明
を行う。マグネット2の基板lとの対向面には、第1図
(b)に示すごとく、N極、S極か交互に配されるごと
く着磁されている。本実施例では8極に着磁され出力パ
ルスの幅角0゜は 2sin−’(Hs  / Ho  )もしくは 2sin−’(Hs’/ Ha )である。
In Fig. 1(a), the magnetic flux emitted from magnet 2 is MR
It passes through the substrate l on which the element is formed, and then returns to the magnet 2 through the stator yoke 3 and back through the substrate l. The magnetization curve of the magnet 2 may be a sinusoidal wave, nine trapezoidal waves, etc., and the following description will be made assuming that it is a sinusoidal wave. As shown in FIG. 1(b), the surface of the magnet 2 facing the substrate 1 is magnetized so that north poles and south poles are arranged alternately. In this embodiment, it is magnetized into 8 poles, and the width angle 0° of the output pulse is 2 sin-' (Hs/Ho) or 2 sin-'(Hs'/Ha).

本実施例のエンコーダ装置にあっては、第1図(d)に
示す如<MR素子6.6′を全て直列に接続する。
In the encoder device of this embodiment, all the MR elements 6 and 6' are connected in series as shown in FIG. 1(d).

第1図(d)のMR素子群におけるMR素子6.6′は
互いに幅、長さか異なっており、即ち、飽和磁界かMR
素子6とMR素子6′とで異なる。いまMR素子6′の
長さを交9幅をWとすると、MR素子6の長さはbl、
幅はawで表わすことかてきる。各MR素子6,6′は
第2図に示す信号磁界て、かつピッチp=π/(n+1
)(n= 0.1,2.・・・・・・)て配列する。M
R素子の飽和磁界はマグネット2の信号磁界に対して十
分小さいため、マグネット2の信号磁界に対するMR素
子群の抵抗値変化は第3図(a)に示すとおりになる。
The MR elements 6.6' in the MR element group in FIG.
The element 6 and the MR element 6' are different. Now, if the length of the MR element 6' is the intersection and the width is W, then the length of the MR element 6 is bl,
The width can be expressed as aw. Each MR element 6, 6' has a signal magnetic field shown in FIG. 2 and a pitch p=π/(n+1
) (n = 0.1, 2......). M
Since the saturation magnetic field of the R element is sufficiently smaller than the signal magnetic field of the magnet 2, the resistance value change of the MR element group with respect to the signal magnetic field of the magnet 2 is as shown in FIG. 3(a).

従って、定電流■。をこれらの素子6.・・・・・・出
力パルスの幅角0゜は 2sin−”(Hs /Ho ) もしくは 2sin−’(Hs’/Ho )である。
Therefore, constant current ■. These elements 6. ...The width angle of the output pulse at 0° is 2sin-'' (Hs/Ho) or 2sin-'(Hs'/Ho).

本実施例のエンコーダ装置にあっては、第1図(d)に
示す如<MR素子6,6′を全て直列に接続する。
In the encoder device of this embodiment, the MR elements 6 and 6' are all connected in series as shown in FIG. 1(d).

第1図(d)のMR素子群におけるMR素子6.6′は
互いに幅、長さが異なっており、即ち、飽和磁界がMR
素子6とMR素子6′とで異なる。いまMR素子6′の
長さを文1幅をWとすると、MR素子6の長さはbl、
幅はawで表わすことができる。各MR素子6,6′は
第2図に示す信号磁界で、かつピッチP=π/(n+1
)(n= 0.1,2.・・・・・・)で配列する。M
R素子の飽和磁界はマグネット1の信号磁界に対して十
分小さいため、マグネットlの信号磁界に対するMR素
子群の抵抗値変化は第3図(a)に示すとおりになる。
The MR elements 6.6' in the MR element group in FIG. 1(d) have different widths and lengths, that is, the saturation magnetic field is MR
The element 6 and the MR element 6' are different. Now, if the length of MR element 6' is W and the width of sentence 1 is W, then the length of MR element 6 is bl,
The width can be expressed as aw. Each MR element 6, 6' has a signal magnetic field shown in FIG. 2, and a pitch P=π/(n+1
) (n = 0.1, 2......). M
Since the saturation magnetic field of the R element is sufficiently smaller than the signal magnetic field of the magnet 1, the resistance value change of the MR element group with respect to the signal magnetic field of the magnet 1 is as shown in FIG. 3(a).

従って、定電流I。をこれらの素子6.・・・・・・に
通電すると、同様の出力変化を得ることができる。即ち
、磁界の位相角π/(n + 1)毎にパルス状の出力
が得られ、パルスレベルの異なるパルス状の出力が磁界
の位相角π毎に得られる。こうして得られた出力変化を
示す波形を整形して、矩形波を作る際、その基準電圧を
適宜選択することにより、容易に第3図(b)、第3図
(C)に示す複数種の出力信号を得ることができる。
Therefore, constant current I. These elements 6. A similar output change can be obtained by energizing . That is, a pulse-like output is obtained every phase angle π/(n + 1) of the magnetic field, and a pulse-like output with a different pulse level is obtained every phase angle π of the magnetic field. When shaping the waveform indicating the output change obtained in this way to create a rectangular wave, by appropriately selecting the reference voltage, it is possible to easily generate the multiple types of waves shown in Figures 3(b) and 3(C). You can get the output signal.

また、これは特に幅に限らず、厚み9組成を制御して飽
和磁界を変化せしめ、第3図(a)に示す抵抗値変化が
得られれば、同様の作用を示すことができる。
Further, this is not limited to the width, but the same effect can be obtained if the saturation magnetic field is changed by controlling the thickness 9 composition and the change in resistance value shown in FIG. 3(a) is obtained.

第4図は本発明の第2の実施例としてのエンコーダの構
成を示す断面図てあり、外周部に着磁された円筒状マグ
ネット8に対向する円筒状基板9の内周面にMR素子か
形成されている。該MR素子は上述した第1の実施例の
場合と同様で、第1図(c)に示す信号磁界で、幅、長
さが異なるMR素子6.6′がp=π/ (nil) 
 (n−0゜1.2.・・・・・・)のとッチて配列さ
れ、MR素子6についてはπのピッチで配列される。そ
して、これらMR素子6.6′は全て直列に接続されて
いる。この実施例においても、マグネット8の信号磁界
に対するMR素子の抵抗値変化は第3図(a)、(b)
、(C)のようになる。
FIG. 4 is a sectional view showing the configuration of an encoder as a second embodiment of the present invention, in which an MR element is mounted on the inner circumferential surface of a cylindrical substrate 9 facing a cylindrical magnet 8 magnetized on the outer circumference. It is formed. The MR element is the same as in the first embodiment described above, and in the signal magnetic field shown in FIG. 1(c), the MR element 6.6' with different widths and lengths is
The MR elements 6 are arranged at a pitch of (n-0°1.2...), and the MR elements 6 are arranged at a pitch of π. These MR elements 6.6' are all connected in series. Also in this example, the change in resistance value of the MR element with respect to the signal magnetic field of the magnet 8 is shown in FIGS. 3(a) and 3(b).
, (C).

第5図は本発明の第3の実施例の考え方を示す図である
。本実施例において、マグネット11は直線的に動き、
該マグネットの動きに伴ってMR素子群12より出力パ
ルスを得る。マグネット11はMR素子群12と対向す
る面に図示の如くN極、S極が交互に配される如く着磁
されており、MR素子群12は、長さの異なるMR素子
12aとMR素子12bが直列に接続されたものであり
、これに伴い所定周期でパルス状出力が得られ、かつ該
所定周期より長い周期で幅の異なるパルスが得られる。
FIG. 5 is a diagram showing the concept of the third embodiment of the present invention. In this embodiment, the magnet 11 moves linearly,
Output pulses are obtained from the MR element group 12 as the magnet moves. The magnet 11 is magnetized so that N poles and S poles are alternately arranged as shown in the figure on the surface facing the MR element group 12, and the MR element group 12 has an MR element 12a and an MR element 12b of different lengths. are connected in series, and as a result, a pulse-like output is obtained at a predetermined period, and pulses with different widths are obtained at a period longer than the predetermined period.

上述の如きエンコーダを例えば扁平ブラシレスモータの
速度検出器としてmmいる。これにより、モータのメイ
ンマグネットを被検出マグネ・ントとすることができ、
該マグネットに対向して上述の如きMR素子のパターン
を配せば、速度検出用のマグネットを特別に設ける必要
がなく、モータの小型化及び部品点数の削減が可能とな
る。
The encoder as described above is used, for example, as a speed detector for a flat brushless motor. This allows the main magnet of the motor to be the detected magnet.
If a pattern of MR elements as described above is arranged opposite to the magnet, there is no need to provide a special magnet for speed detection, and the motor can be made smaller and the number of parts can be reduced.

上述の各実施例のエンコーダにおいては、マグネットの
着磁数を増やすことなく、出力パルス数を増加すること
ができ、分解能を容易に高めることが可能となる。また
、同一の出力パルスを得る様に配置された複数組のMR
素子を直列に接続することにより、偏心9着磁ムラ等の
物理的要因に伴う出力信号精度の劣化を低減することが
可能となりだ。
In the encoders of the embodiments described above, the number of output pulses can be increased without increasing the number of magnetized magnets, and the resolution can be easily increased. In addition, multiple sets of MRs arranged to obtain the same output pulse
By connecting the elements in series, it is possible to reduce deterioration in output signal accuracy due to physical factors such as eccentricity and uneven magnetization.

[発明の効果] 以上説明したように、この発明はMR素子の飽和磁界を
所定の規則に従って異にして組合わせることによって、
複数種類の信号を得ることができた。これにより、MR
素子群とそれに対向するマクネットの相対速度が異なる
場合においても、例えばそのMR素子のパターンが所定
周波数の信号とそのに倍の周波数の信号の2種類の周波
数の信号を出すことがてきれば、相対速度がl/kにな
った場合でも同数の周波数の信号を得ることかてきる。
[Effects of the Invention] As explained above, the present invention has different saturation magnetic fields of MR elements according to predetermined rules.
We were able to obtain multiple types of signals. As a result, MR
Even if the relative speeds of the element group and the facing macnet are different, for example, if the pattern of the MR element can output signals of two types of frequencies: a signal of a predetermined frequency and a signal of twice the frequency. , it is possible to obtain signals with the same number of frequencies even when the relative velocity becomes l/k.

また、1つのMR素子群より複数の信号を得られること
から、そのためのパターンを新たに配列することなく、
エンコータの小型化に効果がある。
In addition, since multiple signals can be obtained from one MR element group, there is no need to newly arrange patterns for this purpose.
This is effective in downsizing the encoder.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図(a)、(bつ、(C)、(d)は本発明の第1
の実施例である回転型エンコータについて説明するだめ
の図であり、第1図(a)は断面図、同図(b)、(C
)はマグネットの着磁の様子を示す図、同図(d)はM
R素子のパターンを示す図、第2図は各MR素子より得
られる出力を説明するための図、第3図は本発明のMR
素子の抵抗値変化を示す図、第4図は本発明の第2の実
施例としてのエンコーダの構成を示す断面図、第5図は
本発明の第3の実施例としての直動型エンコーダの考え
方を示す図である。 図中。 l、9:基板  2.8. II:マグネット3.10
:ステータヨーク 4:回転基板  5:回転軸 6.12:MR素子 7:導体 代理人 弁理士 1)北 嵩 晴 (Q) (C) 第1図 第1 図(d) (a) (b) (C) 第3図 第4図 第5図
FIGS. 1(a), (b), (C), and (d) are the first embodiments of the present invention.
FIG. 1(a) is a sectional view, FIG. 1(b), (C
) is a diagram showing how the magnet is magnetized, and (d) of the same diagram is M
A diagram showing the pattern of the R element, FIG. 2 is a diagram for explaining the output obtained from each MR element, and FIG. 3 is a diagram showing the MR element of the present invention.
FIG. 4 is a cross-sectional view showing the configuration of an encoder as a second embodiment of the present invention, and FIG. 5 is a diagram showing a change in resistance value of an element. It is a figure showing a way of thinking. In the figure. l, 9: Substrate 2.8. II: Magnet 3.10
: Stator yoke 4: Rotating board 5: Rotating shaft 6.12: MR element 7: Conductor agent Patent attorney 1) Haru Kitatake (Q) (C) Fig. 1 Fig. 1 (d) (a) (b) (C) Figure 3 Figure 4 Figure 5

Claims (2)

【特許請求の範囲】[Claims] (1)被検出体と検出体の相対位置を検出するエンコー
ダ装置であって、所定ピッチで着磁された被検出体と、
飽和磁界が前記被検出体の着磁磁界に対し十分小さく、
前記着磁ピッチに比し小さいピッチで並列する複数の磁
気抵抗効果素子を前記被検出体に対向させ、前記並列す
る複数の磁気抵抗効果素子の飽和磁界を所定の規則に従
って異ならしめた検出体とを備えたことを特徴としたエ
ンコーダ装置。
(1) An encoder device that detects the relative position of a detected object and a detected object, the detected object being magnetized at a predetermined pitch;
the saturation magnetic field is sufficiently smaller than the magnetizing magnetic field of the detected object;
A detection object in which a plurality of magnetoresistive elements arranged in parallel at a pitch smaller than the magnetization pitch are opposed to the object to be detected, and the saturation magnetic fields of the plurality of magnetoresistive elements arranged in parallel are made different according to a predetermined rule. An encoder device characterized by being equipped with.
(2)並列する複数の磁気抵抗効果素子の幅及び長さ、
または幅もしくは組成を異にしたことを特徴とする特許
請求の範囲第(1)項記載のエンコーダ装置。
(2) Width and length of multiple parallel magnetoresistive elements,
The encoder device according to claim 1, wherein the encoder device has a different width or composition.
JP62300023A 1987-11-30 1987-11-30 Encoder apparatus Pending JPH01142413A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62300023A JPH01142413A (en) 1987-11-30 1987-11-30 Encoder apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62300023A JPH01142413A (en) 1987-11-30 1987-11-30 Encoder apparatus

Publications (1)

Publication Number Publication Date
JPH01142413A true JPH01142413A (en) 1989-06-05

Family

ID=17879778

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62300023A Pending JPH01142413A (en) 1987-11-30 1987-11-30 Encoder apparatus

Country Status (1)

Country Link
JP (1) JPH01142413A (en)

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